One new ingredient of our proof
is the construction of the velocity and magnetic flows
with the refined spatial intermittency,
which are designed specifically to concentrate on small spatial cuboids
and, as the intermittent Mikado flows in [1]},
have mutually disjoint supports.
This particular structure enables us to gain an additional almost
1D spatial intermittency than that in
the ideal MHD case [2]},
and thus to control the fractional viscosity and resistivity \((-\Delta )^{{\alpha }_i}\) 
with \({\alpha }_i \in [0,1)\) , \(i=1,2\) .
